Herschel Calibration Workshop March 25 – 27, 2013 ZeroPoint Correction for Herschel-SPIRE Maps via PlanckHFI Cross Calibration Bernhard Schulz, Luca Conversi with special thanks to Guilaine Lagache, Pedro Gomez, Steve Guest, Gabriele Mainetti, the Planck Team, the SPIRE team, and the HCalSG page ‹#› PACS Herschel Calibration Workshop March 25 – 27, 2013 Overview • Zero-point correction: – Objective, Plan, Change of Plan • • • • • Algorithm for comparison Color correction Derivation of beam profiles HIPE 10 implementation New HIPE 10 products page ‹#› PACS Herschel Calibration Workshop March 25 – 27, 2013 SPIRE/HFI Cross-Calibration The Opportunity The Plan • Herschel-SPIRE 350mm and 500mm filters have strong overlaps with PlanckHFI 857GHz and 545GHz respectively • • Planck-HFI use COBE-FIRAS maps (3% accuracy) to flux-calibrate their maps in these two filters in offset and scale. • • The COBE-FIRAS calibration for the overlapping filters is based on two onboard blackbodies operated in space. • The FIRAS beam is 7°, the HFI beam is 5’, the SPIRE beams are 25” and 36”. Take accurate blackbody calibrated COBE-FIRAS all-sky maps with 7° beam and cross calibrate Planck-HFI 545 and 857 GHz maps with ~5’ beams. Take Planck-HFI 545 and 857 GHz maps, make sure photometric gains match, and correct zero-point of SPIRE maps with 18, 25, 36” beams. HFI-857 PLW PMW HFI-545 PSW page ‹#› PACS Herschel Calibration Workshop March 25 – 27, 2013 Change of Plans • In our first comparisons we found the photometric gains of the FIRAS based HFI maps were considerably higher than those of the SPIRE maps. • Because of this and other inconsistencies the Planck team decided to change the calibration scheme for the 545 and 857 GHz channels. • Change of calibration scheme for Planck-HFI 545 and 857 GHz maps – Derive photometric gain from observations of Uranus and Neptune. – Derive zero levels from correlation of HI (21cm) gas column density and add CIB mean level. – See talk by Guilaine Lagache (Planck Collaboration VIII. 2013, In preparation) page ‹#› PACS Herschel Calibration Workshop March 25 – 27, 2013 Map Comparison (Algorithm) • Derive a color corrected HFI map at the reference wavelength of the SPIRE band based on the flux ratio of both HFI bands. • Convolve SPIRE maps assuming an 8’ Gaussian beam. • Determine first offset estimate and embed SPIRE map into HFI map that is set to SPIRE offset estimate to reduce edge effects. • Repeat convolution and comparison. • Comparison (for photometric verification) – Plot HFI and SPIRE maps pixel by pixel and fit gain and offset. – Determine median and scatter in difference map. Planck simulated map SPIRE embedded + convolved • Correction (for SPIRE pipeline) – Determine median and scatter in difference map. – Add median difference to SPIRE map page ‹#› PACS response function the instrument for T( ν) is the relative spectralSED not only at the of reference ν01 to the real sky spectrum Fwhere document describes aFway( to ν)perform ν sky ( ν). This fixes the flux of thatThis ref Herschel Calibration Workshop and overlapping SPIRE and HFI filterbands tha frequency of the first filter, but Aalso for calibration the secondoffilter. ii) Then the flux at thefilters reference frequency cross two different photometric can be done with ob March 25 – 27, 2013 To correct this flux for the actual spectrum of th without user intervention. ν to the fiducial spectrum. Let be ν02 of the second filter is transferred Fstd ν01asand area onback the sky with knownreference relative This can seen a sequenc N 1 SED. standard Herschel or1 Planck photometer fluxde Introduction 1 ν0 ν T1( ν) dνν0 and ν0 fluxdensities at theFsky reference wavelengths Fstd ν02 be the monochromatic steps: i) first a transfer from 1the fiducial reference1spectrum2 S = const ν ν 0 The Herschel and Planck missions quote thecorrection actual at theSED referen Fsky the respective color factors asthe defined respectively, and let K1 and Kν0 skyof spectrum This of fixes thesky fluxabove.Then of that not o Fsky ( νSED ). 2 be 1 to the real ν flux densities S at a given reference wave N 1 from 1 but also for the second filter. ii) Then the flux a frequency of the first filter, Fsky ( ν ) T1( ν ) dν ν0 1 Fref ( ν) of the second filter is transferred back to the fiducial reference spectru ν0 Fstd ν02 K2 Fsky ν02 2 K F ν0 ν F ν0 1the2sky 2spectrum sky 0 Tofluxdensities correct thisν0 flux forreference actualwavelength follows K12monochromatic = = Fstd ν0 = Fstd the at the Fstd ν02 be 2 1 ν ν0F1 Fsky ν01 ν01 Fstd ν01 K1 K2Planck standard HerschelFsky or f N 1 sky photometer with 1respective F ( ν0 ) K = F ( ν0 ) K and be the color correction factors respectively, and let K K Fsky ν0 2 2 ν T2sky ( ν) dν 1 std actual SED of the sky at the re Fsky of the ν from 0 Color Correction • • • • • Objective: From 857 and 545 GHz maps construct a map as if with , measured with SPIRE. The HFI and SPIRE maps are N 1 Fstd ν02 K2 Fsky νν0 K1 Fsky ν02 2 1 defined at the reference =the F ν02 = Fs so the correction factor from one fluxdensity toν0 other becomes Fskyand ( ν ) Tfollows ( ν )Kdν = 2 2 12 K F std Fsky ν01 Fstd ν01 K1 ν0 wavelengths/frequencies and a F ( ν0 ) K = F ( ν0 ) ν 2 skysky 1 with std 0 where T( ν) is the relative spectral response fun standard reference spectrum. becomes the finally color correction factor becomes The actual spectrum is a cold A cross calibration of two different photometric νN 1 galactic dust spectrum ν spectral respons ( νN) 1is the relative so the correction factor from fluxdensity to the other becomes T1where ( ν)one T area on the sky with known relative SED. This c ν01 dν Fsky( ν) T2 ( ν) dν characterized by a temperature. ν A cross νcalibration of two different photom 0from the ν 0 a transfer steps: i) first fiducial referen Color correction factors are area on the sky with known relative SED. K12 = νN 1 tabulated for a range of νN 1 ( ν) spectrum This fixes ν01 to the realTsky F from ( ν).the i) first a transfer fiducial re 2steps: temperatures. dν ν02 3 Fsky( ν) sky T1 ( ν) dν νν0 to the real sky spectrum F ). This 2 h nu 1 filter, but also for sky the( νseco ν0 Using the Planck flux law B( nu T)frequency νof the first Ratios of monochromatic 0 h nu frequency of the first filter, but also for filter is transferred back to the th ν02 of the second densities in the HFI map are 2 kb T The sky SED is of the second filter is transferred back ν0 c e 1 2betwen HFI and SPIRE Color Correction Factors tabulated for the same list of monochromatic fluxdensities Fstd ν02 be the 3 fluxdensa Fstd ν02 be the monochromatic 1.8 2the h nu we will calculate the color corrrection factors for practical cas nu temperatures. we define the relative sky SED as In theF following Using B( nu T) with ( nu T)the Planck B( nu T)law and be the rest respectively, and let K K fluxessky measured with the two highest frequency filters of Planck-HFI into fluxes h nu and be the respecti respectively, and let K K GHz 1 2 1 filters. It 2is assumed that the com correspond to the overlapping Herschel-SPIRE 2 kb T from c e 1 corresponding skybins of regridded maps that have from An alternative to the SED based on the Planck law could be a simple power spectrum of the formbeen convolved to the same must be larger or at least equal to the instrument with K the smaller Fstd ν0 Fsky spatial ν02 resolut 1.8 2 2 nu b = we define the relative sky SED as F ( nu T ) B ( nu T ) nu Fstd ν02 K ν02 F ν0 GHzHl fo sky K Hs2 F Fν0 sky Fsky_p( nu b ) M Jy 1 sky 1 follows std 1 ..\bandpass_857_v1.0.da GHz...\SpirePhotRSRF.txt and the flux ratio is page ‹#› 10 = K Fsky ν01be a simple power spe F ν0 An alternative to the SED law could 1 Planck std based1 on the M reverse ( M ) b PACS Herschel Calibration Workshop March 25 – 27, 2013 Neptune Fine Scan Maps PSW PMW PLW • With background sources. page ‹#› PACS Herschel Calibration Workshop March 25 – 27, 2013 Fitted Background Ecliptic coordinate grid Direction of tilt and strength of gradient are compatible with using a Zodiacal light model by Reach et al. (1996) and extrapolating it to submm wavelengths. • Solution 1: • Fit and subtract a warped background plane (implemented). • Solution 2: • Obtain “shadow” observation and subtract (next version). page ‹#› PACS Herschel Calibration Workshop March 25 – 27, 2013 Neptune Fine Scan Maps PSW r=1000’’ PMW PLW r=700’’ • Maps after removal of background sources. • Coverage beyond 700’’ radius is low and reliability is questionable. page ‹#› PACS 200 400 600 radius [arcsec] 800 0 1000 Herschel Calibration Workshop March 25 – 27, 2013 PMW radial flux average [Jy] (tilt-sub) PSW radial flux average [Jy] (tilt-sub) 100 Sector 1 Sector 2 Sector 3 10-2 10-4 200 400 600 radius [arcsec] 800 1000 0 100 200 400 600 radius [arcsec] 800 1000 100 PLW radial flux average [Jy] (tilt-sub) 0 Sector 1 Sector 2 Sector 3 10-2 10-4 Sector 1 Sector 2 Sector 3 10-2 10-4 After Source and Background Removal 400 600 radius [arcsec] 800 PMW radial average (tilt-sub) PMW radial fluxflux average [Jy][Jy] (tilt-sub) 0 Sector 1 Sector 2 Sector 3 -1•10-4 -1•10-4 0 0 200 200 400 400 600 radius [arcsec] 600 radius [arcsec] 800 800 1000 1000 1•10-4-4 1•10 5•10-5-5 5•10 Background [Jy/beam] = :-8.0E-06 0 0 After background subtraction of [Jy/beam] = :-8.0E-06 -5•10-5-5 -5•10 -1•10-4-4 -1•10 0 200 200 400 600 400 Inner radius600 [arcsec] radius [arcsec] 800 800 1000 1000 1200 462’’2 -5 5•10 460 -1•10-4 0 0 200 200 400 400 600 800 600 800 Integration radius [arcsec] Inner radius [arcsec] 1000 1000 -5•10-5 -5•10-5 1000 0 Sector 1 Sector 2 Sector 3 -4 -1•10 -1•10-4 0 0 200 200 400 400 600 radius [arcsec] 600 radius [arcsec] 800 800 1000 1000 200 400 600 radius [arcsec] 800 1000 5•10-5-5 5•10 Background [Jy/beam] = :-1.8E-05 0 0 After background subtraction of [Jy/beam] = :-1.8E-05 -5•10-5-5 -5•10 -1•10-4-4 -1•10 0 0 200 200 400 400 600 600 Inner radius [arcsec] radius [arcsec] 800 800 1000 1000 1200 825’’2 830 -5 795’’2 8100 Omega(Neptune) [arcsec^2] = : 794.8 +/- 0.3 After background subtraction of [Jy/beam] = :-1.8E-05 200 200 400 600 800 400 Integration radius 600 [arcsec] 800 Inner radius [arcsec] 1000 1000 Background [Jy/beam] = :-2.0E-05 5•10-5 Background [Jy/beam] = :-2.0E-05 1200 1200 3 0 -5•10-5 2 Sector 1 Sector 2 Sector 3 -5•10-5 -1•10-4 0 200 400 0 200 400 600 radius [arcsec] 600 radius [arcsec] 800 1000 800 1000 1•10-4-4 1•10 5•10-5-5 5•10 Background [Jy/beam] = :-2.0E-05 0 0 After background subtraction of [Jy/beam] = :-2.0E-05 -5 -5 -5•10 -5•10 -1•10-4-4 -1•10 0 0 200 200 400 600 400 Inner radius600 [arcsec] radius [arcsec] 800 800 1000 1000 1200 1690’’2 1665’’2 1•10-4 1690 5•10-5 1680 0 1670 Omega(Neptune) [arcsec^2] = :1665.4 +/- 0.2 After background subtraction of [Jy/beam] = :-2.0E-05 -1•10-40 0 200 200 400 600 800 400 Integration 600 radius [arcsec] 800 Inner radius [arcsec] 1000 1000 1200 1200 Removed sources and warped plane improves consistency between three beam sectors. Background estimates similar to previous estimates before source removal. Integration out to 600’’ results in 450’’2, 795’’2, 1665’’2 respectively for PSW, PMW, PLW. Integration out to 1000’’ results in 462’’2, 825’’2, 1690’’2 respectively for PSW, PMW, PLW. Integrated solid angles smaller again. 465 460 455 Omega(Neptune) [arcsec^2] = : 449.5 +/- 0.1 450 0 200 400 600 800 Integration radius [arcsec] 1000 1200 830 820 810 Omega(Neptune) [arcsec^2] = : 794.8 +/- 0.3 800 790 0 200 400 600 800 Integration radius [arcsec] 1000 1200 1 0 1660-5 -5•10 790 -1•10-4 0 0 1•10-4 5•10-5 -1•10-4 1•10-4-4 1•10 800 -5•10-5 1200 1200 800 0 0 5•10 820 After background subtraction = :-8.0E-06 Omega(Neptune) [arcsec^2] = : 449.5of +/-[Jy/beam] 0.1 -5 600 radius [arcsec] Background [Jy/beam] = :-1.8E-05 Background [Jy/beam] = :-1.8E-05 1•10-4 450’’2 0 455 -5•10 450 PSW Integrated Solid Angle [arcsec^2]) 0 PMW Average background outside radius [Jy] PMW radial flux average [Jy] (tilt-sub) -5•10-5 400 1•10-4 5•10-5 5•10-5 PMW Average background outside radius [Jy] PMW Integrated Solid Angle [arcsec^2]) -5•10-5 200 1•10-4 1•10-4 PMW Integrated Solid Angle [arcsec^2]) radial average (tilt-sub) PSWPSW radial fluxflux average [Jy] [Jy] (tilt-sub) 0 1•10-4 465 • • • • • Background [Jy/beam] = :-8.0E-06 Background [Jy/beam] = :-8.0E-06 5•10-5 PSW Average background outside radius [Jy] PSW Integrated Solid Angle [arcsec^2]) PSW background outside radius [Jy] PSWAverage radial flux average [Jy] (tilt-sub) 1•10-4 10-6 10-8 0 1•10-4 5•10-5 10-8 1000 flux average [Jy] (tilt-sub) PLWPLW radialradial flux average [Jy] (tilt-sub) 200 PLW background outside radius [Jy] PLWAverage radial flux average [Jy] (tilt-sub) 0 PLW Average background outside radius [Jy] PLW Integrated Solid Angle [arcsec^2]) 10-8 10-6 PLW Integrated Solid Angle [arcsec^2]) 10-6 1690 1680 Omega(Neptune) [arcsec^2] = :1665.4 +/- 0.2 1670 1660 0 200 400 600 800 Integration radius [arcsec] 1000 1200 page ‹#› PACS Herschel Calibration Workshop March 25 – 27, 2013 SPIRE Extended Source calibration • • • • • • Re-built fine scan map of Neptune with 1 arcsec pixel size. Removed sky background structure (tilt and galaxies) Integrated solid angle to 600” radius. Estimated uncertainty is +/- 4%. Recently (Nov 2012) obtained “shadow” observation of the same region should improve accuracy further. Monochromatic extended source fluxes are quoted assuming the standard ν*Fν=const. reference spectrum. page ‹#› PACS Herschel Calibration Workshop March 25 – 27, 2013 HIPE 10 Implementation • New Healpix Library to read HFI 545 GHz and HFI 857 GHz maps. • Interpolator for irregularly distributed data points. • HIPE task “zeroPointCorrection()” • Input parameters: – Level 2 context with three extended source maps – Two HFI Healpix maps at 545 GHz and 857 GHz. – A table with pre-calculated relative color correction factors based on relative HFI flux ratios and a simple dust model. – Photometric gains (1.0) SPIRE/HFI for 545 GHz and 857 GHz. – SPIRE photometer solid angles (hard coded 465, 822, 1768”^2) – Effective Gaussian FWHM of HFI maps (8’’) page ‹#› PACS Herschel Calibration Workshop March 25 – 27, 2013 Comparison in Detail I PMW or PLW Convolved SPIRE map Solid Angle from Beam Profile Expand Map Convert to MJy/sr multiply by K4ext/K4pnt divide by Solid Angle Convolve Kernel is convolution of 8’ Gaussian and HFI Beam model (Smaller ~3.5’ Gaussian) SPIRE All sky Healpix maps HFI-545 Color Correction HFI-857 Ratio map Color corrected HFI map HFI-545 to PLW HFI-857 to PMW Ratio HFI-857/HFI-545 HFI page ‹#› Color correct HFI map to SPIRE filter bands PSW or PLW based on fit of Grey-Body dust model with β=1.8 to HFI fluxes. PACS Herschel Calibration Workshop March 25 – 27, 2013 Comparison in Detail II Determine median difference. Fit Offset and Scale. Compare within mask Flux SPIRE Map Convolved SPIRE map Color corrected HFI map Embed SPIRE map into median adjusted HFI map Embedded SPIRE map Flux HFI Map Mask where edge effects <0.1% 1st Scale 1st Offset 1st Median Offset Embedding reduces edge effects in the subsequent SPIRE map convolution page ‹#› PACS Herschel Calibration Workshop March 25 – 27, 2013 Comparison in Detail III Embedded SPIRE map Pipeline Output Convolved SPIRE map Color corrected HFI map Compare within mask Flux SPIRE Map Convolve Determine median difference. Fit Offset and Scale. SPIRE map with corrected zero-point using median difference Flux HFI Map 2nd Scale 2nd Offset 2nd Median Offset Mask for entire SPIRE map Median and standard deviation of the difference map in FITS header page ‹#› PACS Herschel Calibration Workshop March 25 – 27, 2013 Map Correlations First Comparison Second Comparison (embedded map) page ‹#› PACS Herschel Calibration Workshop March 25 – 27, 2013 New last segment of SPIRE standard product generation timelines with sky positions psp product map product diagnostic product psrcPxWdiag destriper Level 2 Level 1 baseline corrected timelines insert destriper map psrcPxW Naïve map ssoPxW ssoMotionCorrection applyRelativeGains destriper extdPxWdiag zeroPointCorrection Planck HFI Maps Gain Factors extdPxW Colour Correction Factors page ‹#› PACS Herschel Calibration Workshop March 25 – 27, 2013 New Level 2 Products • Point source maps [Jy/beam] renamed to psrcP?W. • Associated diagnostic products named psrcP?Wdiag. • (for SSOs) Proper motion corrected maps ssoP?W. • Extended source maps [MJy/sr] with FIRAS/HFI absolute sky background levels extdP?W. • Associated diagnostic products named extdP?Wdiag. page ‹#› PACS Herschel Calibration Workshop March 25 – 27, 2013 Planck-HFI Maps In March 2011 the Planck team kindly agreed to make a confidential release of HFI 545 and 857 GHz maps before the official release date to enable zero-point correction of SPIRE maps in the data reduction pipeline at the Herschel Science Center only. • Subsequently four different internal releases for the HFI 545 GHz and HFI 857 GHz filter bands were received and evaluated – (DR2, DX7, DX9, re-calibrated DX9). • • • Relative photometric gains, consistency and beam profile verifications were conducted. HFI photometry of planets was compared with planet flux models. Regular telecons/meetings of the HFI/SPIRE cross calibration team were held to clarify matters, agree on policies, and to provide feedback to the Planck project. page ‹#› PACS Herschel Calibration Workshop March 25 – 27, 2013 Gain Verification • Verification of the photometric gain is a prerequisite for the zero-point correction of SPIRE photometer maps. • Select large SPIRE photometer maps, re-reduce to Level 1 and construct de-striped maps. • Exclude smaller fields, fields with low flux dynamic range, fields with strong saturated sources close to the edge. • Run comparison procedure. – There are one IDL and two HIPE implementations for cross checking. • Determined ratio of photometric gains for SPIRE and HFI maps from pixel to pixel plots of SPIRE and HFI data. • The scatter of the difference maps is at a few per cent of the respective background flux level. page ‹#› PACS Herschel Calibration Workshop March 25 – 27, 2013 Map Flux Ranges page ‹#› PACS Herschel Calibration Workshop March 25 – 27, 2013 Gain Verification • • A total of 119 large SPIRE maps were included in the comparison. We plot the flux ratios PMW/HFI-857 (top) and PLW/HFI-545 (bottom). • The median ratios are 0.949 and 0.951 with standard deviations 0.009 and 0.011 for PMW/HFI-857 and PLW/HFI-545 respectively. page ‹#› PACS Herschel Calibration Workshop March 25 – 27, 2013 Gain Verification • The HFI fluxes are about 5% brighter than the SPIRE fluxes in both channels. • A similar comparison of several maps by the Planck team yields an average of 2% and 7% brighter HFI fluxes at 545 and 857 GHz (Planck Collaboration VIII. 2013, In preparation). • Although the correspondence between the HFI and SPIRE calibrations is very good, the relative difference between the gains both teams found is significant and we are looking for the reason. page ‹#› PACS Herschel Calibration Workshop March 25 – 27, 2013 HIPE and IDL Results HIPE and IDL gains agree well, on average within 0.4% and 1.7% for PMW and PLW. page ‹#› PACS Herschel Calibration Workshop March 25 – 27, 2013 Summary • The new zero point calibration implementation into HIPE 10 is complete and operational. • • • • • • • The new maps fit into the new Level 2 product structure adopted by SPIRE for HIPE 10. The new Level 2 product structure contains zero-point corrected SPIRE maps in [MJy/sr] and keywords specifying the median and the standard deviation of the difference map. New solid angles for the conversion to extended source fluxes have been determined to an accuracy of 4%. New “shadow” observations will improve the accuracy further and are being analyzed. The current HFI maps are photometrically consistent with the SPIRE maps within the quoted 10% absolute photometric accuracy of the HFI maps. The HFI photometry seems to be biased towards slightly higher fluxes and both teams find different photometric ratios. A more refined analysis is ongoing. page ‹#› PACS
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